Hermitian Operators: Identifying & Solving Examples

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Homework Help Overview

The discussion revolves around identifying Hermitian operators in quantum mechanics, specifically examining the operator \(\hat{A} \psi(x) \equiv \exp(ix) \psi(x)\). Participants are exploring the definition and properties of Hermitian operators.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the mathematical condition for Hermitian operators, questioning how to apply the definition in the context of wavefunctions. There are attempts to express the Hermiticity condition using integrals and inner products.

Discussion Status

The discussion is ongoing, with some participants providing insights into the calculations needed to verify Hermiticity. There is a mix of understanding and confusion, particularly regarding the application of definitions to specific examples.

Contextual Notes

Participants express uncertainty about the calculations involved and the specific application of Hermitian operator definitions to wavefunctions. The original poster indicates a lack of clarity on how to start the problem.

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Homework Statement



I have some operators, and need to figure out which ones are Hermitian (or not).

For example:

1. \hat{A} \psi(x) \equiv exp(ix) \psi(x)

Homework Equations



I have defined the Hermitian Operator:

A_{ab} \equiv A_{ba}^{*}

The Attempt at a Solution



I just don't know where to start with this :rolleyes:
 
Last edited:
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One good way is to see if something is hermitian is if

\langle \psi | A | \psi \rangle= \langle \psi |A| \psi \rangle^*

if A is hermitian then the equality will hold.
 
Ok but I don't understand the calculations to do :rolleyes:
 
The way you expressed the opeator A_{ab}=A*_{ba} is a matrix notation, useful when acting on a set of vectors like v_{b}. But in your problem, how does the operator act on the wavefuntion Psi(x)? Can you re-express your definition above for Hermiticity in this specific case?
 
Umm I have this:

\langle a|\hat{A}|b \rangle = \int dV \psi_{a}^{*}(r)r^{2}\psi_{b}(r)=[\langle b|\hat{A}|a \rangle]^{*}

But I don't know if that's any use
 
Still don't get this :frown:
 
So, for example

\hat{A} \psi(x) \equiv exp(ix) \psi(x)

\langle \psi | A | \psi \rangle= \int \psi^*(x) exp(ix) \psi(x)

\langle \psi | A | \psi \rangle^*= \int \psi^*(x) exp(ix)^* \psi(x)=\int \psi^*(x) exp(-ix) \psi(x) \neq \int \psi^*(x) exp(ix) \psi(x)

The operator is not hermitian.
 

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